Exact(5)
This is because we assumed that only the reflection coefficient of the simulated materials depends on the wavelength, while the remaining parameters are constant (see Table 1).
Finally, the implemented software framework was used to homogenize a measured distortion map produced by a single PET module by superimposing distortion corrections from additional simulated materials.
Table 1 Properties of simulated materials Young's modulus (N/mm) Poisson's ratio Cancellous bone 1370 0.30 Cortical bone 13700 0.26 PDL 0.6668 0.49 Tooth 20000 0.30 Bracket and SS wire 214000 0.30.
Models with variable gap distances with an interval of lattice constant increment of the simulated materials are set up and statistical comparisons of temperature evolution curves are made.
It was found that for Knudsen and free molecular diffusion in the simulated materials, the Deff/Vt vs. SSA graphic nearly follows a power law.
Similar(55)
Figure 9 The division into stripes in direction Y of a section of the simulated material.
Assume that m geometrical quantities (underline{X}=[X_{1}, ldots, X_{m}]') are measured for each available section of the simulated material.
Each section both of the real and the simulated material is represented by an image having dimension (200times240) pixels in directions (Xtimes Y).
end{aligned} Figure 10 The division into stripes in direction Y and direction X of a section of the simulated material.
Therefore, both enhancing the mathematical model and defining the simulated material better in the sense of its characteristic coefficients mean reducing the error of the application.
Based on the simulated material flow behavior, the defect formation mechanism is revealed and an avoidance mechanism through the dynamic change of tooling geometry is proposed.
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